US 20110075964 A1
A system and method for monitoring the structural integrity of a structure is provided. An optical fiber is acoustically coupled to one or more of the structural elements. A source of optical energy is configured to inject optical energy into the optical fiber, and an optical detector is configured to detect a first optical return signal having characteristics that are affected by vibrations of the structural elements. An analyzer measures characteristics of the optical return signal to determine information concerning the movement of the structural elements monitored by the fiber optic cable. The results of the analyzer can be stored and so that the analysis of the optical return signal can be compared to previously recorded signals to determine changes in structural integrity over time. Multiple fibers can be acoustically coupled to the monitored structural elements to obtain additional data concerning the structural integrity.
1. A system for monitoring a structure having a plurality of structural elements, the system comprising:
a first optical fiber acoustically coupled via a gel to at least one of the plurality of structural elements;
a first source of optical energy configured to inject optical energy into the first optical fiber;
a first optical detector configured to detect a first optical return signal having characteristics determined at least in part by vibrations of the at least one of the plurality of structural elements;
an analyzer configured to determine a first information concerning a structural integrity of the at least one of the plurality of structural elements based at least on a comparison of the characteristics of the first optical return signal to a plurality of known optical return signal characteristics.
2. The system of
a storage device storing the characteristics of a plurality of previous optical return signals detected by the first optical detector,
wherein the known optical return signal characteristics include the stored characteristics of the plurality of previous optical return signals.
3. The system of
a second fiber acoustically coupled via the gel to at least one of the plurality of structural elements;
a second source of optical energy configured to inject optical energy into the second optical fiber; and
a second optical detector configured to detect a second optical return signal having characteristics determined at least in part by vibrations of the at least one of the plurality of structural elements;
wherein the analyzer is further configured to determine a second information concerning the structural integrity of the plurality of structural elements based at least on a comparison of the characteristics of the second optical return signal to the plurality of known optical return signal characteristics.
4. The system of
5. The system of
6. The system of
7. The system of
8. The system of
9. The system of
10. A method for monitoring a structure having a plurality of structural elements, the method comprising:
injecting optical energy into a first optical fiber acoustically coupled via a gel to at least one of the plurality of structural elements;
receiving from the first optical fiber a first optical return signal having characteristics determined at least in part by vibrations of the at least one of the plurality of structural elements;
comparing the characteristics of the first optical return signal to a plurality of known optical return signal characteristics; and
determining a first information concerning the structural integrity of the at least one of the plurality of structural elements based at least on a result of the comparison of the first optical return signal and the plurality of known optical return signal characteristics.
11. The method of
storing the characteristics of a plurality of previous optical return signals received,
wherein the known optical return signal characteristics include the stored characteristics of the plurality of previous optical return signals.
12. The method of
injecting optical energy into a second optical fiber acoustically coupled via the gel to at least one of the plurality of structural elements;
receiving from the second optical fiber a second optical return signal having characteristics determined at least in part by vibrations of the at least one of the plurality of structural elements;
comparing the characteristics of the second optical return signal to the plurality of known optical return signal characteristics; and
determining a second information concerning the structural integrity of the at least one of the plurality of structural elements based at least on a result of the comparison of the second optical return signal and the plurality of known optical return signal characteristics
13. The method of
14. The method of
15. The method of
16. The method of
17. The method of
18. The method of
19. The method of
The present disclosure relates to optical fiber surveillance systems and methods, and more particularly to methods and systems for monitoring structures and structural integrity using optical fiber surveillance systems.
As buildings, bridges and other structures age, the structural integrity of those structures begins to decline. To ensure such structures to not fail, engineers and architects incorporate a factor of safety into designs. However, a factor of safety can not prevent the gradual erosion of structural integrity that occurs over time or the impact of man-made accidents or natural disasters. Structural integrity can be monitored by measuring the deformation of movement of buildings over time. Similarly, strain and stress gages can be applied to or built into buildings. However, these measurements are limited to the specific points or elements measured and do not provide a broad and detailed view of the integrity of the entirety of the structure.
In accordance with an embodiment of the present disclosure, a system for monitoring a structure having a plurality of structural elements is provided. An optical fiber is acoustically coupled to one or more of the structural elements, and a source of optical energy is configured to inject optical energy into the optical fiber. An optical detector is configured to detect an optical return signal having characteristics that are affected by vibrations of the one or more of the plurality of structural elements. An appropriately configured analyzer can then be used to analyze the characteristics of the optical return signal to determine information concerning the movement of the one or more structural elements monitored by the fiber optic cable.
In a further feature of the present disclosure, the results of the analyzer can be stored in a storage device. The analyzer can then compare information concerning the movement of the monitored structural elements to the previously recorded movements. The comparison can further be made with respect to the movement of the monitored structural elements over time based on multiple recorded previous results.
Multiple fibers can be acoustically coupled to the monitored structural elements to obtain additional data concerning the structural integrity. Each fiber can be provided with its own source of optical energy and optical detector. The analyzer can be further configured to determine information concerning the movement of the monitored structural elements based on the characteristics of the optical return signal from the additional fibers. Alternatively, a separate analyzer can be provided for each fiber.
The monitoring fibers can be coupled to the monitored structure using a gel for better transmission of vibrations. If the optical fiber is routed through a conduit, the gel can be used to fill the conduit. Alternatively, if the fiber is acoustically coupled to the exterior of the structural element, a U-channel can be used to hold the fiber in place and filled with the gel to acoustically couple the fiber to the structure.
These and other advantages of the present disclosure will be apparent to those of ordinary skill in the art by reference to the following detailed description and the accompanying drawings.
In one aspect of the present disclosure, the remote fiber surveillance configuration can include a wireless transmitter 105 having an appropriate antenna 106 that transmits a signal to a wireless receiver 107 with appropriate antenna 108. Thus, the remote fiber surveillance system can be deployed in one location and monitored from a different location, optionally in real time, without requiring wired communication with the source 103 and detector 105. For example, the surveillance system could be deployed along various pipelines in Alaska and Texas, but both deployments could be monitored from a central monitoring station in Colorado. It would be understood by one having ordinary skill in the art that antennae 106 and 108, as well as the transmitter 105 and receiver 107 can be of any appropriate configuration and technology for transmitting and receiving wireless signals respectively. The wireless transmitter 105, receiver 107, and antennae 106 and 108 can involve any over-the-air transmission technology. It will be further understood that the analysis instrumentalities can be included in either transmitter 105 and/or receiver 107 and that either or both can be connected to appropriate storage media to save data prior to or after processing. The wireless transmissions can occur continuously to provide continuous monitoring or, in a “sometimes-on” embodiment, can occur periodically or at selected times
In an alternative embodiment of the present disclosure, multiple fibers, such as those illustrated in
The fiber topology illustrated in
In the embodiment of
It will be noted that in the two dimensional topology of
Another further application of the disclosed technology is shown in
As discussed above, many fiber surveillance technologies determine the location of the disturbance based only on the distance along the fiber of the detected disturbance. This determination is most often made by measuring signal strength as a function of distance along the fiber, as measured for example by delay between the time that the source optical signal is injected into the fiber and the time that the reflected signal is detected. However, when the orientation of the fiber is two-dimensional rather than one dimensional, the exact location (e.g., geographic location, location along a pipeline, etc.) of any point along the fiber may not be known. Accordingly, the location of a disturbance may not be determinable simply based on the distance along the fiber where the disturbance is located. Therefore, it would be advantageous to know the location of points along the fiber as a function of its distance of the points along the fiber. The location of points along the fiber can be determined by imposing a vibration or other acoustic signal at known points along the fiber. In this way, the location of the fiber can be mapped and the distance along the fiber can be associated with a specific location. Such characterization of the fiber location can be accomplished by using, for example, well-known crystal controlled vibrating rods. As the rod is moved relative to the fiber, both along the fiber and perpendicular to it, the signal will be maximum when the rod is exactly over the fiber. In this way, the fiber may be calibrated to determine the exact location of any point along the fiber.
In accordance with a further feature of the present disclosure, not only can the location of a disturbance be determined, but if the source of the disturbance moves, its location can be determined at different times. Accordingly, the path of travel and the velocity of motion, as well as other characteristics of the motion, can be determined. In alternative embodiments of the present disclosure, this information can be used to provide advanced warning not only of unauthorized activity, but of impending collisions between moving objects or between a moving a stationary objects.
In accordance with an embodiment of the present disclosure, the fiber surveillance system can be used to monitor structures, such as buildings and bridges. The disturbances discussed above result in vibrations (i.e., acoustic energy), therefore just as disturbances can be monitored by the present disclosure, vibrations within a structure or propagated by a structure can be used to monitor the structure. Furthermore, vibrations in a structure can be used to determine characteristics regarding the structural integrity of a structure.
During installation, fiber 510 can be blown through a section of a conduit 520 using installation techniques known to one of ordinary skill in the art. In this manner, a fiber 510 can be blown through the interior of several miles of structure 500, depending on the weight and size of the fiber cable. It would be understood by a person of ordinary skill in the art that a single fiber can be used to monitor multiple structural elements. Additionally, multiple fibers can be used to monitor a single structural element. As discussed above, multiple fibers can be installed in a structure in a mesh or other multi-dimensional layout to more precisely locate disturbances and vibrations.
In order to provide better acoustic conductivity between the fiber 510 and the structure 500, the conduit 520 is preferably filled with a gel that increases transmission of vibrational energy from the structure 500 to the fiber 510. One such gel is the “IceFree Antifreeze Gel System,” manufactured by American Polywater Corporation. Liquids (e.g., water) and/or solidifying substances (i.e., materials that can be injected into the conduit as liquid and solidify over time) can be used in place of gel 530. However, gel 530 can provide the additional advantages of being selected to ensure that the substance inside the conduit does not freeze in colder weather. While the fiber could be embedded directly in a concrete structure, expansion and contraction of the concrete and/or shifting of the concrete structure can improperly attenuate the fiber 510.
In yet a further feature of the present disclosure, and as illustrated in
Because the embodiments illustrated in
Structural integrity (e.g., as measured by stress, strain, shear, movement, vibrations, etc) in a structure can be monitored over time. That is, the current signal from the monitoring optical fiber can be compared to one or more previous signals to determine which components are experience undesirable or decreased structural integrity.
The x-axis of histograms 610 and 610′ represents the distance along the length of the fiber which can be measure as described above with reference to
The y-axis of histograms 610 and 610′ represent a characteristic of the signal received from the fiber optic cable. The characteristics can include amplitude, phase-shift, signal beat phase, frequency, and other known properties. For illustrative purposes, the y-axis of
The baseline histogram 610 can be determined in a number of ways. It can represent a measure of the signal characteristic after initial installation or an average over a time period after installation. Alternatively, the baseline histogram 610 can be a sample or average that was measured over a predetermined past time (e.g., an average over a month as measured six months ago). In yet a further alternative, the baseline histogram 610 can be a moving average of the most recent measurements. Other known measures of sampling can also be used.
Each bar of the current histogram 610′ can be compared to the corresponding bar of the baseline histogram 610. As illustrated, a comparison of the histograms 610 and 610′ show that the signal from the fiber segment corresponding to section 620 and 620′ has remained relatively constant. Similarly, the signal from the fiber segment corresponding to section 660 and 660′ has remained relatively constant. In contrast, the signal from the fiber segments corresponding to sections 630 and 630′, 640 and 640′, and 650 and 650′ have increase as compare to their respective baselines. This increase can indicate a decrease in structural integrity of the building corresponding to those fiber segments.
At step 740, the return signal is analyzed to determine the various characteristics that can be used to detect vibrations and movement, as described herein. The results of the analysis can be stored at step 750. The stored results can optionally be incorporated into the baseline measurements used for comparison (e.g., the baseline histogram 610′). The process 700 preferably continues to gather data regarding structure integrity and returns to step 710 to repeat steps 710-750.
At step 760, the results of the analysis at step 750 are compared to the previously stored results. One example of this comparison is illustrated above with respect to
A high-level block diagram of a computer that may be used to implement the methodology of
It would be understood by those having ordinary skill in the art that the present disclosure can be implemented with any appropriate optical scattering technique, including but not limited to Raleigh scattering and OTDR, and/or any optical signal analysis technique useful in optical surveillance systems
As discussed above, optical pulses can be launched into a buried optical fiber and the signal backscattered by the fiber can be detected. The optical frequency of one pulse within a pair of pulses differs slightly from the optical frequency of the other pulse within the pair of pulses. This frequency difference (or separation) itself varies from one pair of pulses to the next. This variation in frequency difference results in a detected backscattered signal having a phase that is modulated by an acoustic signal in the vicinity of the fiber, allowing decoding of the disturbance with improved signal to noise ratio, reduced fading and a linear output.
In the present disclosure, the following definitions apply: The pulses may be considered as individual pulses, pairs of pulses or groups of pulses; The term “launching” includes introducing the pulse into the fiber or transmitting the pulse in the fiber; The term “optical” as used herein may refer to the region of the electromagnetic spectrum that is visible, generally considered to be between approximately 380 nm and 760 nm. However, depending on the application, the term “optical” as used herein can extend into what is sometimes referred to as the infrared and ultraviolet range of the spectrum, for example from 200 nm to 5,000 nm, or 10 nm to 100,000 nm. In any event, the term “optical” will apply to any frequency which is used to transmit data or voice in or through optical fibers; and while the discussion is in terms of an optical fiber, in alternative embodiments pulses outside the optical spectrum may be launched into any appropriate medium that will transmit the pulses.
Where the pulses are 20 meters wide, the frequency difference is on the order of 5 MHz and varies by about 5 MHz from one pulse pair to the next. In alternative embodiments, the frequency difference can range from approximately 1 MHz to approximately 5 MHz. For these parameters, each pulse pair results in independent scattering, yielding improved signal to noise ratio. These parameters also result in a relative phase shift of the interference between pulses within each pulse pair on the order of Pi, yielding reduced fading if multiple pulse pairs are used. (Note that it is possible to detect the scattering of each pulse pair from the same section of fiber to within the spatial width of the pulse.)
Both the amplitude and the phase of the beat signal are affected by acoustic disturbances that may be present in the vicinity of the fiber. In one embodiment, the amplitude and phase is extracted from the scattered signal using known complex demodulation techniques. Demodulation is performed at the known frequency difference between pulses in a pair. Such demodulation may be performed by multiplying the reflected signal at the difference frequency by the sine and cosine of the difference frequency. This results in both sinusoidal components and a DC component. For a specific embodiment, a low pass filter with cut-off frequency in the vicinity of 5 MHz isolates the DC component. (Note that if this low pass filter is too narrow it will blur the spatial resolution of the result and if it is too broad it will include the results from the next pair of pulses that may be separated by about 10 MHz yielding a result that is not independent.) The DC component reflects the phase and amplitude of the scattered signal. Rectangular to polar conversion enables the independent determination of the phase and amplitude. The phase will drift relative to the local demodulating signal because of small, slow-varying, changes in environmental parameters. Accordingly, to remove this drift, a high pass filter is used on the phase signal after the rectangular to polar conversion. In this way, only the acoustic signal is observed. Detection techniques that only measure the amplitude suffer from low signal to noise ratio, fading and nonlinearity. The present disclosure, by using pulse pairs with appropriate frequency spacing and by analyzing the phase of the scattered beat signal, results in improved signal to noise ratio, reduced fading, and an output that is linear over a larger dynamic range.
The discussion to this point has focused on a single pulse pair that is transmitted through the fiber. If, for this single pulse pair, we want to look at every 20 meters of fiber, we sample accordingly in time, knowing the time of launch. In analyzing the results, N analysis “bins” may be used, one bin for each 20 meter section of fiber. When multiple pulse pairs are used at some pulse repetition rate then for each bin data will arrive at the pulse repetition rate. A filter is applied to limit the signal to the acoustic band of interest—usually between 1 Hz and 200 Hz for acoustic coupling through the ground or other solid structure. A low pulse repetition frequency limits the maximum acoustic frequency that can be detected without aliasing. A given frequency difference cannot be reused in a second pulse pair until we have observed all of the backscattering from that frequency difference. Accordingly, a given frequency difference cannot be reused until the round trip time within the cable passes. A 2.5 kHz pulse repetition rate is compatible with a cable length of about 25 miles.
There is still an amplitude variation in the observed signal and if the amplitude gets too low, the signal to noise ratio is poor. In those circumstances, the low amplitude result may be disregarded or given low weight. Additionally, a phase unwrap algorithm may be used to obtain greater dynamic range. Because of the discontinuity in arctan as the phase exceeds the range −Pi to +Pi, it is advantageous to add the results at the discontinuity to remove that artifact. If there is no acoustic disturbance, there is no change in the phase and amplitude. If there is an acoustic disturbance, it results in very small local changes in fiber length and a linear change in the phase reflecting linear strain in the fiber.
The duty cycle may be improved by launching pulse pairs with different frequency deltas for the various pulse pairs. In this way, multiple pairs may be propagated in the fiber at one time and their signals can be differentiated by observing the appropriate deltas. The analysis for a second pulse pair is the same as that described above for the first pulse pair except that the demodulating frequency is the new delta. After the high pass filtered phase result is obtained, it is combined with the appropriate bin from the previous pulse—using a time shift reflecting the time difference between the first and second pulse pair. The resultant acoustic signals will add coherently. That is, if the acoustic signal is varying, the detected variation between the first and second pulse pairs will be in phase and add constructively resulting in improved signal to noise ratio. Additionally, if one of the results for the first pulse pair is faded or has low amplitude, the results for the second pulse pair is highly unlikely to show similar effects because of the pi shift in the deltas.
The foregoing Detailed Description is to be understood as being in every respect illustrative and exemplary, but not restrictive, and the scope of the invention disclosed herein is not to be determined from the Detailed Description, but rather from the claims as interpreted according to the full breadth permitted by the patent laws. It is to be understood that the embodiments shown and described herein are only illustrative of the principles of the present disclosure and that various modifications may be implemented by those skilled in the art without departing from the scope and spirit of the invention. Those skilled in the art could implement various other feature combinations without departing from the scope and spirit of the invention.